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Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET PDF Download

Introduction

  • Cayley-Hamilton Theorem is quite an important theorem used in matrix theory.
  • The Cayley Hamilton Theorem states that all real and complex square matrices will satisfy their own characteristic polynomial equation. This implies that when a square matrix is transformed into a polynomial, then this polynomial will be equal to 0.
  • It is a very important result that is used in advanced linear algebra to simplify linear transformations.

What is Cayley Hamilton Theorem?

  • According to the Cayley-Hamilton theorem, a square matrix will satisfy its own characteristic polynomial equation. 
  • A characteristic polynomial is associated with the determinant of a matrix and the eigenvalues of the matrix will be the roots of this polynomial. 
  • Suppose a square matrix A is given with n rows and n columns. 
  • The characteristic polynomial of this matrix is given as det(λIₙ – A). 
    Here, Iₙ is the identity matrix, λ is a scalar quantity and det signifies the determinant operation.

Cayley Hamilton Theorem Statement

Cayley Hamilton Theorem Statement

p(A) = Aⁿ + aₙ₋₁Aⁿ⁻¹ + ... + a₁A + a₀Iₙ = 0
(OR)
p(A) = 0, where A is an n x n square matrix

  • The Cayley-Hamilton theorem states that the characteristic polynomial expression of a real or complex square matrix will be equal to the zero matrix. 
  • The characteristic polynomial p(λ) = det(λIₙ – A) can be decomposed as p(λ) = aₙλⁿ + aₙ₋₁λⁿ⁻¹ + ... + a₁λ + a₀
    This is a monic polynomial where the leading coefficient, i.e., the coefficient of the highest degree variable, will be equal to 1. 
    Thus, aₙ = 1. Here, aₙ₋₁, ..., a₁, a₀ are coefficients of the variables λⁿ⁻¹, ..., λ¹, λ⁰ respectively.

We have:
p(λ) = aₙλⁿ + aₙ₋₁λⁿ⁻¹ + ... + a₁λ + a₀
p(λ) = λⁿ + aₙ₋₁λⁿ⁻¹ + ... + a₁λ + a₀

On replacing λ with the matrix A, the polynomial can be written as follows:

p(A) = Aⁿ + aₙ₋₁Aⁿ⁻¹ + ... + a₁A + a₀Iₙ

Now according to the Cayley Hamilton Theorem, this polynomial will be 0.
Thus, p(A) = Aⁿ + aₙ₋₁Aⁿ⁻¹ + ... + a₁A + a₀Iₙ = 0 or p(A) = 0

Cayley Hamilton Theorem Formula

  • The Cayley Hamilton theorem formula is extremely useful in performing complicated calculations with speed and accuracy. It can also be used to determine the inverse of a matrix. The formula is given as follows:
  • Suppose the characteristic polynomial of an n × n square matrix, A, is given as:
    p(λ) = λⁿ + aₙ₋₁λⁿ⁻¹ + ... + a₁λ + a₀
    Then,
    p(A) = Aⁿ + aₙ₋₁Aⁿ⁻¹ + ... + a₁A + a₀Iₙ = 0
    Thus, p(A) = 0.
    To determine the inverse, multiply this equation with A⁻¹:
    Aⁿ⁻¹ + aₙ₋₁Aⁿ⁻² + ... + a₁Iₙ + a₀A⁻¹ = 0
    A⁻¹ = - (Aⁿ⁻¹ + aₙ₋₁Aⁿ⁻² + ... + a₁Iₙ) / a₀

Solved Examples

The examples based on Cayley Hamilton theorem are illustrated below:
Example 1 :  Prove Cayley Hamilton theorem for the following matrix?

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Sol:  Let A = Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Let us find characteristic polynomial of given matrix.

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

In order to prove the statement of Cayley Hamilton theorem for A, we need to show that:

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

P(A) = O, hence Cayley Hamilton theorem for given matrix A is proved.

Example 2 : If Cayley Hamilton theorem holds for the matrix, then find its inverse.

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Its characteristic polynomial is -

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

According to Cayley Hamilton theorem -

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Therefore, equation (1) becomes - 

 

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics | Physics for IIT JAM, UGC - NET, CSIR NET

Applications

  • Cayley Hamilton theorem is widely applicable in many fields not only related to mathematics, but in other scientific fields too. 
  • This theorem is used all over in linear algebra
  • One can easily find inverse of a matrix using Cayley Hamilton theorem. 
  • It also plays an important role in solving ordinary differential equations
  • This theorem is quite useful in physics also. Cayley Hamilton theorem plays a vital role in computer programming and coding
    In a newer subject - Rheology, where behaviour of material is studied, this theorem is used to determine the equations that illustrate nature of materials.
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FAQs on Cayley-Hamilton Theorem - Mathematical Methods of Physics, UGC - NET Physics - Physics for IIT JAM, UGC - NET, CSIR NET

1. What is the Cayley-Hamilton Theorem?
Ans. The Cayley-Hamilton Theorem states that every square matrix satisfies its own characteristic equation. In other words, if A is a square matrix and det(A - λI) is the characteristic equation of A, then substituting A for λ in the equation will result in the zero matrix.
2. What is the importance of the Cayley-Hamilton Theorem in mathematical methods of physics?
Ans. The Cayley-Hamilton Theorem plays a crucial role in mathematical methods of physics because it provides a powerful tool for solving linear differential equations and analyzing the behavior of dynamical systems. By applying the theorem, one can obtain a simple expression for the powers of a matrix, which is useful in various areas of physics, including quantum mechanics and classical mechanics.
3. How can the Cayley-Hamilton Theorem be used in UGC-NET Physics exam?
Ans. In the UGC-NET Physics exam, the Cayley-Hamilton Theorem can be used to solve problems related to linear algebra and matrix theory. It can help in finding the eigenvalues and eigenvectors of a given matrix, determining the diagonalizability of a matrix, and solving systems of linear equations. Familiarity with the theorem and its applications can greatly enhance one's ability to solve mathematical problems in the exam.
4. Are there any limitations or conditions to apply the Cayley-Hamilton Theorem?
Ans. Yes, there are certain conditions that must be satisfied to apply the Cayley-Hamilton Theorem. Firstly, the matrix must be square. Secondly, the matrix must have a characteristic equation, which means it must be possible to compute its determinant. Additionally, the theorem assumes that the matrix is defined over a field, which is a mathematical structure with certain properties. These conditions need to be fulfilled for the theorem to be applicable.
5. Can you provide an example of how the Cayley-Hamilton Theorem can be used in physics?
Ans. Certainly! Let's consider a system described by a matrix A. If we want to find the time evolution of this system, we can write down the differential equation dX/dt = AX, where X is the state vector. By applying the Cayley-Hamilton Theorem to the matrix A, we can express A^2, A^3, and higher powers of A in terms of A and its eigenvalues. This allows us to solve the differential equation and determine the behavior of the system over time, which is essential in physics to study various dynamical phenomena.
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